SCIENTIFIC ABSTRACT SHCHELKIN, K.I. - SHCHELKUNOV, S.I.

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SCIENTIFIC ABSTRACT
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0 67483 S oV/ 9- L_- - 59 - 5- 10/ A+ AUTHOR: Shchelkin, K,I, (Moscow) TITLE: A Possible Mechanism for-the 0~7 Intensification of Weak Shock Waves in the Turbulent CorPL-ustion Zone (The Theory of High-frequency Vibrations cf Flames) PERIODICAL: Izvestiya Akademii nauk SSSR, Otdeleniye teld-michesk:Lkh nauk, Energetika. i airtomati-ka, 11959,Nr 5, pp 86-96 (USSR) ABSTRACT: The paper is a continuation of previous work (Ref 1)~ An analytical relationship is obtained between the dimensionless change in pressure in a weak shock wave and the dimensionless increase lin combustion velocity arising in an idealised combustion chamberlof a reactive engine. Special attention is given to the dependence of C3 the intensity of the shock wave on combustion propa.gation It is velocity and vice versa. shown quantitatively that the movement of a shock wave through the combustion zone causes an increase in the -~relocity of turbulent combustion. A criterion is laid down for the intensifi- cation of weak shoc_~z -%,raves in t't,e combustion zone, Card equivalent to a condition for the establishment of high frequency vibrations in the ideal-ised combustion chamber There are 6 figures and 1+ &Dviet references. SUBMITTED: July 16, 1959. V DENIJOV, Yu.N.; 'IRUSHIN, Ya.K.; SHCHELKIN, K-I- Analogy between combustion in an explosion wave and in a rocket motor. Izv. AN SSSR. Otd. tekh. naak. Ener-jy. i avtom. no.6:79-89 X-D 159. (MIRA 13-8) 1. Institut khimichesicoy fiziki AN SSSR i Institut khimicheskoy kinetiki i gorenlya Sibirskogo otdeleniya AN SSSR. (Rockets (Aeronautics)-Gomb-ustion) "T OR Sh(-'-,el',.i:-,, K. I. TITI-M: T%:o Cp-.-,es of Urmt-,6)le volgo -or-eni,ya) PTRIODIC.*J, 7,hur,;~d eks T:en' a-1 Vol 31-~ I Ur 21, -Pp 6oo s --v /rl- 6 - 32 - -: 56 CombuAion (Dva slun,ialra neustoychi- Inny i teorcti.,-'Ic~c'-oy fi:-i,,,iy "C r) - (,o6 ( 1,77 3 T C T Ti:e first part of fie!.! :-, with the unsten3ines-S .-,)f the i7nition front i- - -!,-Iuor,-'tion wave. The aut~,.or first illvc-sti-~,ten a ste-dy ~s-.!torz--Aion wmve. If tl~e adiabatic cx.,ansion of the ~-ns (aft-r n docrease of .--~.s 2.ncrensos the retv..rd!?--tion of t!-,e i.,nition by -- tluamtity of the orcler of mn~--njtule (or 1~.y ~--,)re~ of the retardation it- self, rn,,,, initi--il rurvature of t~-(-- rrort increaz;ps nn-' a 2tea,ly fr:--)nt becomcn unstep~!y. A crit;-%rion is de(?uced for t',-.P- un-:-tea,liness of t'~,, pl-re i-,--ition zone in tY,, detor-~Ztion v e : (E/RTA 1 -T/TA )>, 1. T,)i~: e-,ii~tion c--?i be ~:,ritt--~n C a r d 1 4 Tvio C, tr- e P of T'n -!. -C,~l Coi-.h A i or, 3, (I,-') Y E denotes the activation ener,--y of 'the r.--action, R the con_,tant, i~ - the pres-ure, T the t e -mporn t tire of the non- burnt 1-as :ifter its expansion. The index A ap,arontly de- notes th.:! front of thf- shoc!- wave, tl-.e in-lex J - t'ne Z!-.ur-,'~(, points This criterion cnn easily be applied to any concrete case. The front of the shock ,-.,ave is disturbed if tre i.-nition front becomes unsteady, and this fact catises thi-1 fDr-ation of inclined compreso-ion jumpv,. If the breadth of the front of the detonation wave A/ is small with respect to thr' tilbe dia,71eter (3, many inclined jumps can occ~ir in the plane of the front and in the whole crosE! section of the ti-II-e. T, 'S cross section contains (d/7.X)2 inclined jumi~s which, frorri the SUrface of the shock -.,iave, propa '~faate in various directions ~_s - ve S and i,~nite th,-, ~~ in the in(~lined -shock 7- and especially in thc_- pl,lces of t'-.-ir colli.,,,ion, The front of t*- 'e detonation ,.1,,ave, tl-.erefore, assu-!:.s the sha~pe of a pUls"Itin- bri,~sh. There is a region of siAn deto-ations 2,3, etc, "heais" t h. tion nn.d the de- (-olovr,) bet-re-ten c. one-on' -i;in dr, _t Ca: d 2/'4 tonation v-it~,. i front (brlif7`i), From t',,- ~O-Ove -le-Itioned Two Cases of Fn:-a `, 1 ~ C c:-, 1, u ~ t _~ r~ r 7~ Jiscus~!ion a conflition for t-.iD occurre ce of a "one-hean' spin" can 110 .1cluced: 3X/d = 3t (D-W)/d~l, ;.,here W de-, notes the vi~locit- of Mhe :-as in the co77:pression JU7,P., d - Vie of the tube, D - t'le velor-ity of the detonation, u!u~tr-tdint-n~t of tl~e i,-Inition comDression zone -n(I. a fine structure of t!:e (loton,'Ition front can be. obo~!;(_,rved !ilso in t1i., il-Aon:Aion of co:npres:-ed explosives. - spin deton.-.tion vies, ho,.%,ev~.,r, not in co:,ipresqed explosives, Ti.e "brussh-li"e" structure of the combustion zone in, V~e detoni4lion of exulosives crin Capparently be expl:L-inel 1:,,I, t".e un2teadiness of the p1nne zoll.e of i.-nition an;,; b:,~ Vic Cor-1-Ition of ..imy inc-lined 11-c% waves whic.-. colli-.4e with one anot',er and iEnitc- t,,e ex.plosiv~t. The Second !)art of this n:.er de-ds iyit~-. the unstpnadine~:s of t)ie i-nition 2nne as source of hi-,h frequency con-Ijustion vibr;itions in forced combuction c'na:~,Ihers. 11 criterion il~ zi-ven for L,.e unfiten-11iness of t'.e ulane i-iiition zon-2, 2'.Iso in thin- case, pulsntions of t'e co-,.ibt1-.--tion zone %re cn~.ced by t~.c ~,t_adines- of the w:-ve front. T-.e fre-_~,ency of tl-.c-.-e pul:-_ntionrl. c~,n Ipe estimated 1--y beans of a formula 3// At S :Iron in oref~.-.ure (,.,dthin Eiver in thi ~ ~, -or _10 Two C-i.~es of Ur..lta~-lo Co~-ibu.,;tion ST.T?.,4ITTED t1le incr,--ace in volu7~-2. Tiere a-re Soviet, the travelin- wave) can in e~ti-,2tpd accordiri~l to P ~lu.--Ust 26, l.")58, presour.~~ or !re 6 fi-lires ---nner be whefe -,E d e not e F: ccmb%~tion in ..:- con7tant -.2.0r, and, 7 refei-ences, 6 of Card 4/4 pq N irI 28374 S/124/61/ooo/oo8/tig/042 jV-0 A001/AlOl AUTHORS: Denisov, Yu.N., Troshin, Ya.K,, SYLchelkin, Kj, TITLE: On a certain analoi~y between burnin,;, in a rocket en,:ine and in a detonati.on wave PERIODICAL; Referativnyy zhurnal. Mekhanika, no. 8, 1961, 36, abstract 8B221 (V sb. "3-ye Vses. soveshchaniye po teorii. goreniya. T,1". Moscow, 1960, 193 - 199) TEXT: Without considering physico-chemical processes in the combustion chamber of a rocket enCine, the authors identify the burning zone in the rocket. engine chamber with the zone of strong discontinuity in which a substance goes over from the initial state into the final state at the expense of energy libera- tion. The state of perfect gas formed at fuel evaporation is assumed for the initial state. In this schematization, operational conditions of rocket engines are represented by Gugonio adiabatic curve (its lower branch). Based on a cer- tain analogy of burning in a rocket engine and in a detonation wave, the aathors apply to burning in the rocket engine the criterion of instability of the plane front of burning at detonation Card 1/2 On a certain analogy ... 2f- 374 S/124/61/000/008/019/042 AOOI/AlOl d _( L T dT- (where&T is gas temperature change in the disturbance zone), delay of ignition'C is connected with temperature by the equation 't = ~XRT , These relations, to- gether with the Gugonio adiabatic curve with heat supply q, yield the following condition for excitation in the rocket engine of oscillations with frequency (d/2 ~_)2: E M2,q (7-_ 1)2 2 1 T I Here (,and ~_are certain delay time and width of the burning zone, d is chamber diameter, M1 is Mach number for gas before the burning zone. K_ Artamonov [Abstracter's note: Complete translation] Card 2/2 r1 68860 AUTHOR: Shchelkin, K. I., Corresponding S/030/60/000/02/002/040 Member-6T-the-fLS USSR B008/BO14 TITLE: Detonation Processes PERIODICAL: Vestnik Akademii nauk SSSR, 1960, Nr 2, pp 12-20 (USSR) ABSTRACTt In this article the author reports on the study of detonation pro- cesses and describes the development of the detonation theory.1 First, he explains the fundamental principles of this theory (Figs 1 and 2), which was later completed by Ya. B. Zelldovich (Fig This theory which has been developed for gases is successfully applied to the detonation of condensed explosives. Its reliability in calculating detonations of explosives was improved by the de- velopment of a theoretically founded equation of state for the explosion products. Numerous empirical formulas were replaced by this equation which was derived by L. D. Landau and K. P. Stanyukovich. In spite of the apparent perfection of the detonatior theory it was not possible to explain an experimentally proyed fact identified by the British scientists Campbell and Woodhead in 1926 as a spin detonation with the help of the scheme of a plaau detonation (Fig 4). For comparison, the author shows a normal det- Card 1/3 onation in figure 5. The spin was later detected also in other Detonation Processes 68860 S1030V60100010210021040 B008/ ~0014 slowly reacting mixtures by Kh. A. Rakipova, Ya. K. Troshin, and the author of the article under review. The author showed (Ref 2) that the spin nucleus represents an oblique (discontinuous) shook wave in which the mixture detonates much more easily than in a plane wave, as a result of higher temperature and pressure. An oblique detonation is schematically represented in figure 6. The spin detonation as a detonation directed by the oblique compression shock could be sufficiently founded. Yu. 1. Denisov and Ya. K. Troshin assume that the angle K in figure 6 may assume the shape shown in figure 7. The attempt was made to apply the classical theory of plane detonation to spin detonation. The rate of spin detonation, the state and the velocity of the combustion products could be determined approximately. Determination of the reaction zone of a spin detonation as a three-dimensional process can be facilitated by transforming this problem into a two-dimensional one. Figure 8 illustrates a "normal" detonation which gives a reticular impression and in which a similar event as in the ause of spin detonation was detected. In connection with these experi- ments the author performed an approximate quantitative analysis of the unsteadiness of a plane detonation wave (Ref 4). It was Card 2/3 found that the intensity of the detonation is increased by this 6886o Detonation Processes S/030/60/000/02/002/040 B008/BO14 unsteadiness due to the formation of zones with higher temperatures than those of the plane wave. These zones are reliable detonation centers. The unsteadiness of one type of detonation causes new steadier types. The practical application of the detonation theory is illustrated by the author by the combustion\\processes taking place in rocket chambers (Fig 9). There are 9 figures and 5 Soviet references. ,,ard 3/3 28348 s/124/61/000/007/010/044 A052/A101 Vc.1in, B. P., Troshin, Ya. K., Pilatov, G. I., Shchelkin, K. I. '_MEJ On the reacton-kinetic nature of heterogeneities In the shock front and the part played by them In the process of propagation of gas detonabion FtRIODICAL- Referativnyy zhurnal, Mekhanika, no. 7, 1961, 7, abstract 7B47 Nn. prikl. mekhan. i tekhr.. fiz" no. 2, 1960, 78-89) TEO-' The process of origination of heterogeneities in the for-ward front of a flat detonation layer Is consa-dered theoretically. The disturbance develop:i in thz! ignlt,.on front and propagates over the front with the velocity cf sol.Lr-d in the shock-compressed gas a,. In the direction of propagation of ""n,? disturbance is drifted ty the flow behind the forward shock front acid overtaki%~5 the front at the moment t ~ A a (D - LU wld-,r. of detonation zone, Dthe velocity of detonation, LO - the 'Card 1/3 04" 28348 S1 124/6 1/o(Yj/w7/o io/044 On the rea,:'.I:,r-kInetIc nature ... A052/AIOI of shock-compressed gas in -the laboratory system of coordinates. By ?:I~Iz moment t the disturbance over the ignition front will have the diameter T D 2 (T - I)/(y + I) 'r D I - I/ V 217(7 - IT wretle NL - tne- period of the Induction of ignition, cp/cv - the ratio of sp _~o 1 f 1 ~2 he ats, ~ - 0.5 1, 0. 4 at -e - 1. 4 1 1. 3. The Identif ica-tion of 4 y w~t.r, the i-xper Imen tally obser"ied dimension of heterogeneities enablos or's to :0.1'.sid-ar equatlon (1) as the depindence of the mean dimension of such hetero- ga-.eiti~)s on ren,-tic-n-kinetic and gas-dynamic factors. The results of experi- 11tie track impri:-.,t-_q of detonation wave on faceplates ooverod with a ihin layer of carlbon black are described, Another Pr3c.f nas .~oand of rhe exiStence of Iteterogene., ties, not only near the wall d,,'_o~ation Kibe, b",A over the wholt4 surface of the detonatIon front In Ijbes az- is shown that sz;ch heterogeneities exist also in the Cph?r?i,--al d-toi-.atlon wave. it Is found out that the total number of heterogene- cver 'he whole detrxiatlon -Iront increases with the surfaco of the front. a-i7hor_~ at a ---oncl--islon that spherical detonation, like the gas ts P.41s-zi.ing one, chat hcterogenelties in its front emerge _~,cid rnat. these heterogeneities are not conna-;t6d with the presence ~~ard 2/3 ~K 2'30 S/124/61/000/007/010/044 On the reacton-kinetic nature ... A052/A101 of walls of the detonation container. To bring the fact of multiplication of pulsations with the increase of the surface of detonation front in agreement with the periodical mechanism of detonation, the authors consider it necessary to complement the conception of the mechanism of detonation combustion, given in another study (Denisov, Yu. N., Troshin, Ya. K. Zh. prikl. mekhan. I tekhn. fiz. no. 1, 1960. by Introducing Into the detonation cycle one more link of Instability being the source of emergence of breaks In the shock front. A criterion of the limit of existence of the spin and pulsating detonations is also given. There are 23 references. Yu. Denisov [Abstracter's note: Complete translation] Card 3/3 SHCHELEILN', K.I. Penetrating into the interior of the atom and its nucleus. Friroda 5C no.](':11-22 0 'r1. (MIRA 14:9) 1. Chlen-korrespondent AN SSSR. (Nuclear physics) SECILI'LKIN, K.I. Proof of the im-oossibility of strong deflagrations followed by ,,teak detonations. Dok-1. --M SSSR 139 no.2:420-423 -'l 161. 14:7) 1. lnstitu'u khimicheskoy fiziki AA' SSSR. Chlen-korrespondent All SSSR. (Shock waves) SHCI=IN, K.I. Strange particles. Priroda 51 no.12:10-18 D 162. (MIRA 15:12) 1. Chlen-korres ondent AN SSSR. fFarticles (Ruclear physics)) SERBINCIV., A.I.; TROSHIN, Ya.K.; SHCHELKIN,__K.I. Kinetic parameters of the processes of detonation, spontaneous ignition., and isothermal oxidation of benzene. Dokl.All SSSR 145 no.6:1314-1317 Ag 162. (MEU 15:8) 1. Institut khiTnicheskoy MI SSSR (for Shchelkin). (Benzene) fiziki A14 SSSR. 2. Chlen-korrespondent (Gombustion) -aligHELKIN, Kiri.-Il Ivanovich; FODOSHVINA, V.A., red.; FROPOVA, (Physics of the microcosm; popylar essays] Fizika miklomira; popyliarnye ocherki. Moskva, Gosatomizdat, 1963. 166 p. (MIRA 16:5) 1. Chlen-korrespondent Akademii nauk SSSR (for Shchelkia). (Nuclear physics) ~AH4036542 BOOK EXPLnITATION S/ Shchelkin, Xirill Ivanovich; Trnshin, Ynkov Kirillovich Gas dynamics of combustion (Cazodinamika poreniva). Moscow, 1zd-Vo AN 555R, 1963. 254 p. illus., bfHtn., plates. alto in- sertcd. 3000 copies printed. ,TOPIC TArSt gas detonation, pnR explosion, gas combustion, rocket engine , jet enrine . pas deflarratlon, 11uponint curve, combustion chamber, -flame acceleration PURPOSE AND COVERAGE: This book is intended for scientific workers and engineers interested in the conbustion and detonation of pases, for students specializing In the physics and dynamics of pas and combustion. It may also he of interest to scientific workers. engineers, and specialists In let and rocket engines. The book was written on the basis of the authnrst research work from 1953 to 1962 at the Institute of Chenical Physics, Academy of Sciences SSSR. The classical theory of combustion and detonatinit necessary for the understandinR of new materials is presented. Wo-rka of other Soviet- ;Card I IV~ AM4036542 and non-Soviet authors in this field are cited. Tie book contains 181 diagrams and photos. TABLE OF CONTVNTS: Foreword -- 3 Ch. 1. Detonation 13 1. Tntroductinn 13 2. Classical detonation theorv 14 3. Kinetics of the chenicat reaction and the instability of the plane ignition front in detonntion -- 26 4. Gisdvnnmics of inhomogeneity in the detonation front -- 32 5. Pulsating detonation (exnerimental facts) -- 44 6. Spinning detonation -- 50 7. Nonuniformities and time of chemical reactionseDetonation linits -- 53 S. Conclusions -- 57 Card 2 _. 3-HCHELKIN, K,, r,,, ALIKHAPIOV, A. I., akademik (Nutstanding physicist of our times; the sixtieth birthday- anniversary of I. V. Kurcbatov. Priroda 52 no.1*25-34 163. (MIRA 16-1) _L, --korresponclent AN SSSR (for Shchel-kin),- (Kurchatov, Igor' Vasil`evich, 1903-1960) OYSSAR, E. [Oissaar, F.] (Tallin); SHCHELKIN, K.I. (Moski,a) What is vacuLLm? Priroda 52. no.10:125-126 163.. (IERA 16: 12) 1. Chlen-korrespondent AN SSSR (for ShcheLkin). SH-=ELKIIN, K.I. Derona,.on ~To be conLlnued). lr;rirc~;-a ! I'D Z~ . (:.'T~Lk -17:7) 1. Cialen-korrespondent, A-. SSSR. ACCESSION NR: AP4040961 S/0020/64/156/005/1178/1181 AUTHOR: Shchelkin, K. I. TITLE: High-frequency pulsations in the combustion of solid fuels iSOURCE: AN SSSR. Doklady*, v. 156, no. 5, 1964, 1178-1181 i ~TOPIC TAGS: solid propellant combustion, high frequency oscillation,: .combustion oscillation theory, solid propellant, combustion insta- lbility, rocket fuel ~ABSTRACT: A theoretical study has been made of the causes of the ,initiation and intensification of high-frequency oscillations in solid fuel combustion. Bas'ed on published theo'ries, conditions were !found for the initiation and for the intensification of high-frequency joscillations in the gas evolved and in the solid,fuel surface. Oscil- :lations are absent under following conditions: Ru2P2MG c 2 constant, T mn 4P9 ,where R radius of the grain. uT rate of combustion of the solid 'fuel density of the solid fuelpg - densityaf the gas evolved from the soUd fuel -1 ~6 Card . . . !ACCESSION NR: AP4040961 thermal diffusivity of the gas evolved root of the Bessel 1equation, m and n are the tangential and r;d7mN wave numbers, and C4 - sound velocity in the combustion products. The oscillations are, initiated when one of the parameters in this equation is changed; in ! ;Ithis case the oscillations may be prevented by changing the other ,parameterse The intensification of the high-frequency oscillations is described by the followEng ex- ,in the combustion of solid fuels pression: c2p T 3 q >1 Y (c3 + C4)c2Pr ;where )CIC4, p. are the same as in the above equation, c 3 sound P# velocity in the unburned gas C velocity of the longitudinal sound' :wave in the solid q rat o of the heat release to the initial'-... fuel, M ; !intarnal energy of the unburned gas. Orig. art. has: 18 formulas* JASSOCIATIONt Institut khimichesk'oy fiziki Akademii nauk SSSR Academy of Sciences SSSR) ,(Institute of Chemical Physics, Cara 2/3 ACCESSION NR; AP4040961 SUBMITTEDt 2lFeb64 ,:'SUB CODE: FP ATD PRESS: 3o44 ENCL: do NO REF SOV: 004 OTHERt 002 Card 3/3, ST!GLEIL-H I: ) ~'4 i-_-, 11 -- A, V. A., rz~d. - - ~ -,L - I ~ I '-~y s i c : I I N L ~- . of the mic-ntccsz. po~ulari zed I -~ 4 Z - -, -, populi -;t-nye ocherki. Mcskva, At,.)rnizdat, 1~---5. 230 F, . 1~ (',.'IFA 18:10) 1. .41, SSS,, (for Shchelkin). SHCHELKIff, K.I. (Moskva) To-tonatlon in gases. Friroda 54 nc.8:53-55 AF '6c. j d t, %TT F,~ 1 " - 2 '- c 1: 1. ',;hlen-korrespondent AN SSSR. . ~ F-I 'I , I ~ ( "", , -i ; v ~ ! *" 'i :-,. 1 4, ~ :n ~ ~ - ~i n. p ~: r IFwr -~- r I -- v I '1l , ; . : c~ I , -~ r 4 . 1 1:1 , I -' 1 , ' - I I , I " '. ." , i --. r, - I , , I " . v 0 r ~ r ,;,, ` r i . I ', I I ,L, (.kl:-,-'A 19511) :, A... ", .I, L 106718-66 EWT(m)/T WW-/JW/WE ACC NR: AP6005859 SOURCE CODE: UR/0053/65/087/002/0273/0302 AUTHOR: Shchelkin_.,_K. I_. ORG: none B TITLE: Instability in combustion and detonation of gases SOURCE: Uspekbi fizicheskikh nauk, v. 87, no. 2, 1965, 273-302 TOPIC TAGS: combustion gas dynamics, detonation kinetics, combustion instability ABSTRACT: This paper is a brief survey 9f the experimental and theoretical litera- i ture on conditions of instability in various types of combustion and detonation of gases. The general theory of normal combustion is outlined and dimensionless formu-j las are given for determining conditions of instability in this type of combustion* ~!.. Experimental data are given an diffusion combustion and the accompanying phenomenon. . of instability in a plane flame.front., The theoretical basis of detonation is dis-'_ :cussed and formulas are given for determining the instability of a plane gas deto nation with respect to deformation of the combustion fr*nt. One-dimensional detona"! UDC: 534.222.2+536.46 Card 1/2 Card 2/2 1, o L -25710-00' ACC NR: AP6010553 SOURCE CODE: UR/0026/65/000/011/0113/0114 AUTHOR.1L_Bhc4pjki_n,,. K, (Corresponding member AN SSSR) 1;2 ORG: none T=-. Inspi-rea -life of Academician 1. :9. Tamm SOURCE: Priroda, no. 11, 1965, 113-114 TOPIC TAGS: physics personnel, particle physics ABSTRACT: The life of Academician Igor' Yevgeniyevich Tamm is described on the occasion of bis 70th birthday. 14511owing are the essential fea- tures of this biography. He was born Tuly 8, 1895, in Vladivostok. His general education was obtained in the Elizavetgrad (now Kirovograd) gymnasium. In 1913, he was admitted to the Edinburgh University (Scot- land) but, in 1914, returned to Russia and entered the University of Moscow. In 1915, he voluntarily entered the military service and serv- ed as a hospital attendant. In 1917, he was elected to the Elizavetgrad Soviet and was sent., as a delegate, to the first Convention of Soviets in Petrograd. After graduation, he taught physics (1921-1922) in the Odessa Polytechnic Institute and in 1922 returned to the Moscow Univer- sity. In 1934, he became head of the theoretical department of the Institute of Physics of AN SSSR im. P. N. Lebedev (EILNIand has held Card I /P L 25710-66 ACC NRz AP6010553 -3 this office up to the present time. In 1945, he presented a method (based on the quantum mechanics) for solution of problems of meson physics. This method is similar to that proposed in 1950 by Dancoff in U.3.A. Thus, it was called the Tamm-Dancoff method. He predicted (together with S. A. Alltshuller) the existence of magnetic moment in neutron. In 1950, he proposed (together with A. D. Sakharov) a method---.:~' for plasma confinement by magnetic field. In 1958~, he received (wit.*a P. A. Cerenkov and I. M. Frank) the Nobel Prize for his theoretical study of the coherent radiation caused in a medium. by a fast moving electron (Cerenkov radiation). He also was bestowed many high Soviet awards. Detailed information on his works and scientific achievements were,given in the publications of V. L. Ginzburg, Ye. L. Feynberg and A. D. gakhax27-,- These publications were ci d in the present RMcle. Orig. art. has: 1 photo. SHCHEIKIN, V.P., inzh. ". !IWI!r Saturation choke with phase control. Trudy MAI no.85.'5-22 157. (Magnetic amplifiers) (KLRA 10:9) PUD('VIX, A.11.; SH CULKI)[A, L.P.; RASHIROVA, L.A. Substitution reaction of phosphoacetic ester and phosphoacetone. Zhur. ob. khim. 27 no.9-2367-2371 S '57. (MIRA 11:3) l.Kazanski7 gosudarstvennyy universitet. (Acetic acid) (Acetone) AUTHORS: TITLE: PERIODICAL: S/08 62/000/004/060/087 B1 50YB1 36 Liorber, P. G., Shchelkina, Ye. P., Deychmeyster, m. V., Vompe, A. F. Some merocyaninocarbocyanine derivatives of imidazolinone-, (4) Referativnyy zhurnal. Khimiya, no. 4, 1~62, 456, abstractl 4L416 (Tr. Vses. ri-i. kinofoto-instituta, no. 37, 1960, 5-16) TEXT: Symmetrical and asymmetrical merocyaninocarbocyanine derivatives are synthesized from 1-cyclohexyl-3-methylimidazolinone-4 with the residues of various heterocyclic bases in merocyanic and carbocyanic components of the molecule. An investigation is made of the structural dependence of the colors of these compounds and of the nature of the clectron density distribution in the chromophores of the molecule. 1A bstracter's note: Complete translation Card 1/1 17- 3- GAYDAMAK, S., student; SIMLINYAKOVA, G., studentka; HZ'HINti, F., _-tudentl